Technically, we used earlier established works
[1]}, [2]}, [3]} for screened interaction energy
in order to model a new (regularized Coulombic) adjustable dissipative channel which
could model the sudden ionizing role of lattice ions in the many-body system of electrons at random
collisional condition in transmission. Concretely, in [4]} we derived
\(\frac{1}{v}\, \frac{dE}{dx}\, =\, \left[Q^{(1)}(v_F)\, + Q^{(2)}(v_F)\right],\) 
